Three-dimensional x-ray imaging with Fourier reconstruction

• US 20060204070A1
• Filed: 03/05/2005
• Published: 09/14/2006
• Est. Priority Date: 03/05/2005
• Status: Abandoned Application

• Current Assignee: Waldo S. Hinshaw
• Original Assignee: Waldo S. Hinshaw
• Inventors: Hinshaw, Waldo S.
• Application Number:
  US10/906,769
• Publication Number:
  US 20060204070A1
• Time in Patent Office: Days
• US Class Current: 382/132
• CPC Class Codes: G06T 11/006 Inverse problem, transformation from projection-space into object-space, e.g. transform methods, back-projection, algebraic methods

Abstract

This invention is a method of generating images of the interior of an object through the use of x-rays or other radiation that is attenuated upon passing through the object. This technology is known as computed tomography, or CT. In the prior art, the x-ray source is moved around or over the object while the r-ray attenuation is observed at multiple locations of the source and while the object stays within the beam of x-rays. The current invention is an efficient method of generating images of the interior of an object by passing the object in a straight line between an x-ray source and a two-dimensional detector array. As the object passes from one side of the cone-beam of x-rays to the other, each detector element records a one-dimensional parallel-ray projection of a slice of the object. The projections so obtained are Fourier transformed and added into Fourier-space according to the projection-slice theorem. Images of the interior of the object are then obtained by taking the inverse Fourier transform of the data in Fourier-space. This method of imaging has the deficiency that results from incompletely populated Fourier-space. The spatial resolution in one direction can depend upon the spatial resolution in another direction. This is the same deficiency suffered by tomosynthesis, an important prior art method of CT. With the current invention, the deficiency can be removed by taking additional projections with the object in a different orientation. Except for the motion of the object, this invention is a CT imaging system with no moving parts.

Claims

1. A method of obtaining images of the distribution of an internal property of a selected volume of an object, said method comprising the steps of:

irradiating the selected volume with multiple rays of energy that are produced and detected by an assembly consisting of a localized energy source and a detector array said energy source and detector array being spatially fixed with respect to each other;

moving the selected volume through the assembly between the energy source and detector array or allowing the selected volume to move through the assembly or moving the assembly over the selected volume, the relative motion being in a substantially straight line and the motion being such that the selected volume is substantially outside of the assembly both at the beginning and end of the motion;

recording the location of the selected volume relative to the assembly and for each location recording the intensities of the rays that have passed through the object and have been attenuated by said internal property and have been detected by the detector array;

calculating the attenuation from the recorded intensities and computing the Fourier transforms of said attenuation as a function of the recorded location, said Fourier transforms being called F-components;

placing said F-components as lines of numbers or planes of numbers into an intermediate array; and

obtaining an image by taking a Fourier transform of the numbers in the intermediate array.

2. A method according to claim 1, in which the said detector array is a two-dimensional array.

3. A method according to claim 1, in which the said detector array is a one-dimensional array.

4. A method according to claim 1, in which the said intermediate array is a two-dimensional array and into which the F-components are placed as lines of numbers, said F-components having been derived from the rays going through a slice of the selected volume.

5. A method according to claim 4, in which images of two-dimensional tilted slices are separately obtained, said images then being combined to form a three-dimensional image.

6. A method according to claim 1, in which the said intermediate array is a three-dimensional array and into which the F-components are placed as planes of numbers.

7. A method according to claim 1, in which the numbers in the intermediate array is restricted in one or more directions.

8. A method according to claim 1, in which the numbers in the intermediate array are reduced in amplitude near one or more edges.

9. A method according to claim 1, in which placing F-components into said intermediate array involves the gridding process.

10. A method according to claim 1, in which the detector array is flat and is parallel to the direction of the relative motion of the selected volume.

11. A method according to claim 1, in which the selected volume passes through multiple assemblies or through the same assembly multiple times with the selected volume having a different orientation with respect to the assembly or assemblies during each pass.

12. A method according to claim 11, in which the plane normal to the axis about which the object is reoriented is at the edge of the detector array.

13. A method according to claim 1, in which the initiation and termination of the recording of intensities is coordinated with the location of the selected volume as it passes through the assembly.

14. A method according to claim 1, in which separate intensities are collected for multiple x-ray energies.

15. Apparatus for obtaining images of the distribution of an internal property of a selected volume of an object by recording and processing the intensities of multiple rays that have passed through the selected volume and have been attenuated by the said property, said apparatus comprising:

a means for irradiating the selected volume with multiple rays of energy and detecting the resulting ray intensities, said means being an assembly consisting of a localized energy source and a detector array said energy source and detector array being spatially fixed with respect to each other;

a means for ensuring that the said assembly and selected volume move in a substantially straight line with respect to each other;

a means for recording the relative location of the selected volume with respect to the assembly;

a means for recording the information from the detector array and for taking the Fourier transforms of said information;

a means for placing said Fourier transforms into an intermediate array as lines of numbers or planes of numbers; and

a means for taking the Fourier transform of the numbers in the intermediate array and presenting the resulting images.

16. Apparatus according to claim 15, wherein the said assembly includes either beam defining collimators or scatter reduction collimators.

17. Apparatus according to claim 15, including a means for moving the selected volume with respect to the assembly.

18. Apparatus according to claim 17, wherein the means for moving the selected volume includes a carrier that contains the selected volume.

19. Apparatus according to claim 15, including a means for moving the assembly with respect to the selected volume.

20. Apparatus according to claim 15, wherein the detecting means is a flat two-dimensional array of detector elements that is parallel to the direction of motion of the selected volume relative to the assembly.

21. Apparatus according to claim 15, providing the means for the selected volume to pass through multiple assemblies or the means for the selected volume to pass through the same assembly multiple times, said means giving the selected volume a different orientation with respect to the assembly or assemblies during each pass.